Abstract
The magnetoabsorption of millimeter-wave radiation by single crystals of the organic metals α-(BEDT-TTFTlHg(SCN and α-(BEDT-TTFKHg(SCN has been studied in the frequency range 30–120 GHz. The experiments reveal two dominant contributions to the magnetoabsorption spectra. The first is interpreted as the cyclotron resonance of two-dimensional carriers, and is characterized by broad lines (linewidth/magnetic field ΔB/B∼0.5–1). In addition to a resonance exhibiting a cyclotron mass ∼2.8, there are two further lines corresponding to frequency-dependent cyclotron masses in the ranges ∼(1–1.5) and ∼(0.5–0.8). This frequency dependence is believed to result from many-body effects. The second contribution to the magnetoabsorption is formed by a series of narrow lines with ΔB/B∼0.03–0.1 and amplitudes 5–10 times smaller than the features interpreted as cyclotron resonances. These narrow lines are attributed to a superposition of modes due to antiferromagnetic resonance and conduction-electron-spin resonance (ESR). The feature characteristic of antiferromagnetic resonance is the presence of a mode with a frequency that decreases with increasing magnetic field. The magnetoabsorption structure attributed to ESR consists of a relatively broad maximum upon which a sharp dip is superimposed. This behavior is believed to be analogous to the resonant transparency observed in thin metallic films undergoing ESR. © 1996 The American Physical Society.
- Received 12 February 1996
DOI:https://doi.org/10.1103/PhysRevB.53.12794
©1996 American Physical Society